Many-body properties of quasi-one-dimensional boson gas across a narrow CIR
We study strong interaction effects in a one-dimensional (1D) boson gas across a narrow confinement-induced resonance (CIR). In contrast to the zero-range potential, the 1D two-body interaction in the narrow CIR can be written as a polynomial of derivative δ-function interaction on many-body level....
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Published in | Europhysics letters Vol. 101; no. 4; pp. 40002 - 40007 |
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Main Authors | , |
Format | Journal Article |
Language | English |
Published |
EDP Sciences, IOP Publishing and Società Italiana di Fisica
01.02.2013
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Subjects | |
Online Access | Get full text |
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Summary: | We study strong interaction effects in a one-dimensional (1D) boson gas across a narrow confinement-induced resonance (CIR). In contrast to the zero-range potential, the 1D two-body interaction in the narrow CIR can be written as a polynomial of derivative δ-function interaction on many-body level. Using the asymptotic Bethe ansatz, we find that the low-energy physics of this many-body problem is described by the Tomonaga-Luttinger liquid where the Luttinger parameters are essentially modified by an effective finite-range parameter v. This parameter drastically alters quantum criticality and universal thermodynamics of the gas. In particular, it drives the Tonks-Girardeau (TG) gas from non-mutual Fermi statistics to mutual statistics or to a more exclusive super-TG gas. This novel feature is further discussed in terms of the breathing mode which is experimentally measurable. |
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Bibliography: | publisher-ID:epl15243 istex:C22ED669BF21FAE37AB1B9FDE79A468B62B85F7C ark:/67375/80W-9GNDV4QX-3 |
ISSN: | 0295-5075 1286-4854 |
DOI: | 10.1209/0295-5075/101/40002 |